Asymmetric fluid-structure dynamics in nanoscale imprint lithography
Asymmetric fluid-structure dynamics in nanoscale imprint lithography
Asymmetric fluid-structure dynamics in nanoscale imprint lithography
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length between the clamped-clamped ends of the actuator s<strong>in</strong>ce this length willvary when the actuators push and pull.ALFigure 5.3 Model of actuator for stiffness computationBeam bend<strong>in</strong>g equations approximate the stiffness of the distributedflexure r<strong>in</strong>g for each actuation arm. Each one-third segment of the distributedflexure can be modeled as a fixed-fixed beam as shown <strong>in</strong> Figure 5.4. Equation5.4 describes the bend<strong>in</strong>g of a fixed-fixed beam under a vertical load.FLbhFigure 5.4 Fixed-fixed beamF192EIδz= kδzL=3[5.4]3bhwhere I = . The flexure r<strong>in</strong>g is mach<strong>in</strong>ed from 7075-T6 alum<strong>in</strong>um alloy12with a Young’s modulus, E, of 72Gpa. The median radial length of the flexurer<strong>in</strong>g is 3.5 <strong>in</strong>ches. The flexure r<strong>in</strong>g is 1 <strong>in</strong>ch wide and 50 mils thick. With a total63